|Publication number||US7345723 B2|
|Application number||US 10/908,671|
|Publication date||Mar 18, 2008|
|Filing date||May 22, 2005|
|Priority date||May 24, 2004|
|Also published as||EP1759237A2, EP1759237A4, EP2441580A1, US7545469, US20050264734, US20080129939, WO2005116738A2, WO2005116738A3|
|Publication number||10908671, 908671, US 7345723 B2, US 7345723B2, US-B2-7345723, US7345723 B2, US7345723B2|
|Inventors||Michael G. Robinson, Jianmin Chen, Gary D. Sharp|
|Original Assignee||Colorlink, Inc.|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (14), Non-Patent Citations (1), Referenced by (8), Classifications (17), Legal Events (6)|
|External Links: USPTO, USPTO Assignment, Espacenet|
This application claims priority to U.S. provisional patent application Ser. No. 60/573,910, filed May 24, 2004, entitled “Polarization Compensating Elements Using Durable, Low Elasticity Organic Substrates,” which is hereby incorporated by reference herein.
Disclosed embodiments herein relate to optical devices for use in liquid crystal (LC) display systems, and more particularly to reflective liquid crystal on silicon (LCoS) projection architectures that require panel-only compensation. These embodiments represent optical components that consist of one or more birefringent layers that compensate for residual in-plane and out-of-plane retardation present in the OFF-state of an LC panel. The net retardation of the panel (=Δn·d) is then substantially the vector sum of the two retardance components. When reduced to practice with stretched organic polymer films, these components typically demand high durability and high polarization performance, and as such a low-elasticity organic substrate is preferred, as described in the preceding provisional U.S. patent application Ser. No. 60/573,910, which is hereby incorporated by reference herein.
In projection displays using LCoS or other LC panels, there is a need to compensate residual, OFF-state panel retardance to ensure sufficient contrast performance, because such residual in-plane retardance applied to incident optical rays can cause polarization mixing and lead to OFF-state leakage. In the case of large screen televisions based on LC panel projection, this leakage manifests itself as a bright dark-state and one that is often colored. When displaying dark video content, such leakage is very obvious and undesirable. Removing residual OFF-state retardance of the LC panels, or at least its adverse affect, can be achieved by introducing birefringent elements in front of the panel, which was described by U.S. Patent Publication Ser. No. U.S. 2003/0128320, to Xiang-Dong Mi.
In general, compensators act first to remove residual in-plane OFF-state retardance of the panel, and second to reduce OFF-state light leakage due to the out-of-plane retardance which relates to field-of-view (FOV) performance of the LC layer. Removing the in-plane retardance is important, as it affects all incident light, since it corresponds to the extent to which the LC molecules are not aligned normal to the substrate or not balanced in their orientations when projected onto the panel plane. The substantial out-of-plane retardance alters the polarization state of off-axis rays, and acts to reduce the panel's field-of-view and in non-collimated systems leads again to OFF-state leakage. To get the high contrast demanded of current commercial video projection systems, both in-plane and out-of-plane compensation is desired.
Certain disclosed compensation schemes may be used in reflective systems where the input/output beam separating PBSs do not require additional compensation (e.g., wire grid PBSs) or are compensated separately. Such systems provide that a linear polarization state exists prior to the system analyzer. Specifically, dark state light exiting the input/output beam-separating PBSs has the same linear polarization state as the light entering as a result of the orthogonal analyzing and polarization axes. In transmissive systems, the output analyzer orientation is independent of the polarizer and allows for compensation solutions that produce rotated linear output states.
Disclosed herein are embodiments addressing the compensating of a reflective LC panel with a compensator comprising at least one birefringent layer, where each birefringent layer or the collection of birefringent layers can exhibit uniaxial or biaxial properties. Specific cases include a- and c-plate combinations, single biaxial films, tilted c-plates, and bi-layer compensators comprising two uniaxial layers having their optic axes oriented substantially orthogonally with respect to each other. Compensation of transmissive panels can be achieved by related methods and are also covered by the general methodology of this patent by “unfolding” reflective designs. A stretched organic film may be used as the birefringent layer or layers in the described embodiments. To avoid degradation within the harsh environment of a projection system, compensators using these stretched organic films may be formed as an encapsulated laminate. An exemplary effective organic film is a low-elasticity polyolefin film.
The optical system 100 of
The above description of
Still referring to
Although the present application describes the compensators 102 as being positioned outside the panels 104/106, it is also possible to place the compensators 102 “within” reflective panels 104/106, as is shown in
More specifically, applicants have recognized that from a manufacturing or design stability standpoint, if the in-plane retardance of the compensator 102 (Γr) and the panel 104/106 (Γp) are well-matched, this matching may cause difficulties for maintaining the proper relative orientations. This is due to the sharp changes that can occur in optimal orientations when the retardances of the panel 104/106 and compensator 102 are relatively close. As described in the present application, relative orientations of the compensator 102 and the panel 104/106 can be adjusted to accommodate for differences between panel and compensator retardances. The relationship between the in-plane retardance mismatch, which is the difference between the panel's OFF-state in-plane residual retardance and the compensator's in-plane retardance, and the resulting optimal compensating orientation can be determined mathematically as is described herein.
With the described approach, polarization analysis is simplified because light having the same linear input and exit polarization states from any reflective birefringent network in an LC-panel-based light modulation system, with the LC-panel in its OFF-state, will have a linear polarization of arbitrary orientation at the reflecting interface. A compensator/panel combination creating linear polarization in a single pass—incident on the mirror/reflecting layer of the reflective LC panel—therefore represents an in-plane compensation solution. In mathematical terms, this condition may be expressed as O=L·C·I, where O and I are the output (mirror) and input linear polarizations and where C and L are the head-on transformations associated with the compensator and LC panel respectively. For small retardances, e.g., less than approximately 30 nm for optical systems handling visible light, these transformations can be reversed to give O=C·L·I.
Employing a Poincare sphere (see D. Goldstein, Polarized Light, at ch. 12 (2d ed. 2003), which is hereby incorporated by reference herein) as a means of representing and transforming polarizations, the above expression can be written as follows:
In this Equation 1, as discussed in Goldstein, supra, φ and ε are the conventional orientation and ellipticity angles describing the polarized state transformed from the input polarization by the LC layer 104. Γr and θr are the in-plane retardance and orientation of the compensator 102, and λ is the wavelength of the compensated light. The output polarization is linear if it is orthogonal to the vector (0 0 1), hence the scalar product can be equated to zero in Equation 1.
Equation 1 can be solved to give the following expression relating compensator orientation as a function of retardance:
For the specific case of a vertically aligned LCOS panel, the LC material 104 of the panel is aligned predominantly homeotropically in its low voltage OFF-state, but has a slight tilt (e.g., 7°) off-normal in the plane bisecting the polarizer/analyzer orientations. For typical LC thickness and birefringence, Equation 2 maps the input polarization state (φ, ε)=(0°, 0°) onto the polarization state (0°, 1°), which would be consistent with approximately 3 nm of residual in-plane retardance at an input light wavelength of 550 nm.
In cases where chromatic, non-collimated light is compensated, and perhaps in other embodiments, it is beneficial to choose the retarder's in-plane orientation that more closely aligns to the input polarization.
In further described embodiments of this application, applicants have recognized the advantage in choosing a compensator with an in-plane retardance value Γr that is mismatched, at least to a certain degree, from that of the panel Γp in its OFF-state. In particular, because of the steep slope of the C-curve near the 45° solution 205, where θ1≅θ2≅45°, small variations in compensator or panel retardance in the 45° implementation can cause relatively dramatic shifts in the orientation solutions according to the illustrated C-curve of
Moving away from the 45° solution 205 to other portions of the illustrated C-curve 200 provides better systemic tolerance of variations of retardance values, Γr and Γp, thereby improving the manufacturability of the optical systems in which the disclosed compensators are employed. An exemplary solution range would be in those solutions on the C-curve where the orientation angle θ1 is less than approximately 20° and the orientation angle θ1 is greater than approximately 70° (e.g., in those areas where the C-curve 200 is flattening out). A wider-angle range would be where the orientation angle θ1 is less than approximately 30° and the orientation angle θ1 is greater than approximately 60°. The solutions closer to the 45° solution 205 have the disadvantage of requiring tighter tolerance on the in-plane retardance values in order to maintain the same the optical system components near their optimal orientations.
The above description and specifically Equation 1 describes solutions whereby the in-plane residual retardance of a panel Γp can be compensated in a reflective LC projection system by an optical component that has an in-plane retardance Γr equal to, or greater than, Γr. Although in-plane compensation only may yield sufficient system performance, a more complete solution requires simultaneous out-of-plane panel compensation. The embodiments of this patent therefore consist of creating a compensating component that has one or more birefringent layers that has an in-plane retardance value greater than that of the panel and properties that can offer some (or indeed complete) out-of-plane compensation. This component can then be oriented in accordance with Equation 1 to ensure good in-plane compensation.
The approach of
According to the approach of
Applicants have built upon the known use of a crossed a-plate compensator 700 to compensate the effect of an LC panel's 104/106 out-of-plane retardance and in-plane residual retardance in an efficient and manufacturable way. Specifically, applicants have used novel orientations and retardances of the retarder films 702, 704. These novel orientations and retardances are further explained below.
A compound two-layer compensator 700 made from orthogonally oriented birefringent layers 702, 704 whose retardances differ by Γp can compensate a reflective LC panel's FOV by choosing the average layer retardance to be close to Δn·d. A 45° orientation, coinciding with the compensator retardance being matched with the panel's OFF-state residual retardance, would be a known approach in this regard.
Applicants' novel approach involves choosing a certain retardance difference between the compound compensator's in-plane retardance and the panel's OFF-state residual retardance. In an embodiment, the retardance of the compensator 700 is greater than that of the panel 104/106. Head-on residual panel retardance is then compensated by orienting the part in accordance with Equation 2. It may further be advantageous to place the optic axis of the film with largest retardance closest to the polarization axis of the incoming light. For compensator angles away from 45°, the out-of-plane compensation favors smaller average retardance values. Further, in the case where a mismatched bi-layer compensator is incorporated into a reflective system, optimal performance is obtained when the layer with largest retardance faces away from the panel. The smaller retardance film is then closest the reflective panel.
As will be further described in
With further reference to the transmissive solutions of
Other LC panels that are almost symmetric about the their cell-center planes are those that have minimal residual in-plane OFF-state retardance. An example of this would be a vertically aligned LC mode with very small pre-tilt angle (e.g., <2°) away from the substrate normal. Another example would be a twisted vertically aligned mode where the net projected in-plane retardance is very small.
In these low residual cases, where the transmissive panel is effectively homeotropic in nature, the paired compensators can be brought together on a single side of the panel forming a single compensating element consisting of one or more layers. A single layer can be realized by combining equivalent layers such as two equivalent biaxial films. In this case we can compensate in a conventional way a low residual effectively homeotropic transmissive LC with a matched biaxial film with very low in-plane retardance (effectively a c-plate).
Still referring to the transmissive embodiments of
For transmissive panels having a significant pretilt, the equivalence to an unfolded LC system is lost. However compensation schemes can be derived by first unfolding the reflective case assuming perfect homeotropic alignment and second by tilting the compensator in accordance with the tilt of the LC. By way of example, a simple c-plate can be used to compensate a tilted transmissive vertically aligned nematic LC panel by tilting the plate to align the out-of-plane optic axis of the plate to that of the LC. In practice, the ray deflection at material interfaces should be taken into account making the angle of the plate not match exactly with the LC director.
Solutions can be derived in the case of compensating finite in-plane residual retardance of a transmissive panel with reflective symmetry such as a pi-cell. Unlike in the reflective case, however, only one solution exists where the input and output polarization are the same. In the case of a tilted, vertically aligned LC system, this would be the matched 45° solution. It is possible, however, to rotate the output analyzer in the transmissive system as the polarizer and analyzer are physically separate. Good contrast can therefore be achieved if the output polarization is linear. This is the same condition as for the solution set determined in Equations 1 and 2. Compensators with in-plane retardances greater than the panels' residuals can therefore be used for in-plane compensation assuming rotation of the output analyzer. The analyzer angle for any given solution can be derived using expressions similar to those used in Equation 1.
As described above, field-of-view compensation can then be independently addressed with average retardance values using the equivalence of transmissive to unfolded reflective systems. While the unfolded systems can most easily be applied to systems using crossed a-plates (or other systems not having tilted plates), through design techniques it is possible to develop transmissive systems following many of the reflective architectures described above.
The section headings in this application are provided for consistency with the parts of an application suggested under 37 CFR 1.77 or otherwise to provide organizational cues. These headings shall not limit or characterize the invention(s) set out in any patent claims that may issue from this application. Specifically and by way of example, although the headings may refer to a “Field of the Invention,” the claims should not be limited by the language chosen under this heading to describe the so-called field of the invention. Further, a description of a technology in the “Background” or “Description of Related Art” is not be construed as an admission that technology is prior art to the present application. Neither is the “Summary of the Invention” to be considered as a characterization of the invention(s) set forth in the claims to this application. Further, the reference in these headings to “Invention” in the singular should not be used to argue that there is a single point of novelty claimed in this application. Multiple inventions may be set forth according to the limitations of the multiple claims associated with this patent specification, and the claims accordingly define the invention(s) that are protected thereby. In all instances, the scope of the claims shall be considered on their merits in light of the specification but should not be constrained by the headings included in this application.
Realizations in accordance with the present invention have been described in the context of particular embodiments. These embodiments are meant to be illustrative and not limiting. Many variations, modifications, additions, and improvements are possible. Accordingly, plural instances may be provided for components described herein as a single instance. Boundaries between various components and operations are illustrated in the context of specific configurations. Other allocations of functionality are envisioned and will fall within the scope of claims that follow. Structures and functionality presented as discrete components in the exemplary configurations may be implemented as a combined structure or component. These and other variations, modifications, additions, and improvements may fall within the scope of the invention as defined in the claims that follow.
The compensating stacks described herein may be made from any suitable material such as solid crystals, stretched polymers, liquid crystal polymers, or another material. The liquid crystal polymer can have dual homogeneous alignment, splay alignment (homogeneous/homeotropic) or any suitable alignment. Although the compensated retarder stacks are discussed in the context of color management for projection display, they can be used in a number of applications. These include, among others, color separation for image capture or radiometry, lighting, and near infrared optical communications.
Although several embodiments of the present invention and its advantages have been described in detail, it should be understood that changes, substitutions, transformations, modifications, variations, permutations and alterations may be made therein without departing from the teachings of the present invention, the spirit and the scope of the invention being set forth by the appended claims.
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|U.S. Classification||349/117, 349/113, 349/119|
|International Classification||G02F1/1335, G02F1/13363|
|Cooperative Classification||G02F2413/10, G02F2413/13, G02F1/13363, G02F1/136277, G02F2413/08, G02F2001/133637, G02F2203/02, G02F2413/11, G02F1/133634, G02F2413/12, G02F2413/04|
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